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Updated: Jun 12, 2025

Recombination Dynamics in Thin-film Photovoltaic Materials via Time-resolved Microwave Conductivity
Published on: March 6, 2017
Stochastic Schrödinger equation for hot-carrier dynamics in plasmonic systems
Giulia Dall'Osto1, Mirko Vanzan1,2, Stefano Corni1,3
1Dipartimento di Scienze Chimiche, Università di Padova, Via F. Marzolo 1, 35131 Padova, Italy.
We developed a multiscale method to simulate hot-carrier dynamics in plasmonic systems. This approach reveals how nanoparticle effects enhance charge generation and how relaxation times influence these processes.
Area of Science:
- Computational chemistry
- Quantum mechanics
- Materials science
Background:
- Hot-carrier dynamics in photoexcited plasmonic systems are crucial for applications like CO2 photoreduction.
- Understanding the interplay between quantum and classical effects is essential for designing efficient photocatalysts.
Purpose of the Study:
- To develop and apply a multiscale computational method for studying hot-carrier dynamics.
- To investigate the influence of relaxation (T1) and dephasing (T2) times on charge dynamics.
- To elucidate the role of a metallic nanoparticle in plasmon-driven photoreduction.
Main Methods:
- Coupling open quantum systems theory with real-time ab initio electronic structure calculations.
- Utilizing the Markovian Stochastic Schrödinger equation and ab initio GW/Bethe-Salpeter (BSE) equation.
- Modeling the metallic nanoparticle classically using the polarizable continuum model.
Main Results:
- Observed net hole injection from rhodium to a CHO fragment, enhanced by two orders of magnitude due to the nanocube.
- Demonstrated that nonradiative decay (T1) rapidly decreases charge population.
- Showed that pure dephasing (T2) erases coherent charge injection dynamics.
Conclusions:
- The multiscale method accurately captures hot-carrier dynamics in photoexcited plasmonic systems.
- Metallic nanoparticles significantly enhance charge generation in plasmon-driven reactions.
- Both relaxation and dephasing times play critical roles in controlling charge dynamics and photoreduction efficiency.
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